Title: Creating the Virtual Seismologist
1Creating the Virtual Seismologist
- Tom Heaton, Caltech
- Masumi Yamada, Caltech
- Georgia Cua, Swiss Seismological Service
2Earthquake Alerting a different kind of
prediction
- What if earthquakes were really slow, like the
weather? - We could recognize that an earthquake is
beginning and then broadcast information on its
development on the news. - an earthquake on the San Andreas started
yesterday. Seismologists warn that it may
continue to strengthen into a great earthquake
and they predict that severe shaking will hit
later today.
3If the earthquake is fast, can we be faster?
- Everything must be automated
- Data analysis that a seismologist uses must be
automated - Communications must be automated
- Actions must be automated
- Common sense decision making must be automated
4How would the system work?
- Seismographic Network computers provide estimates
of the location, size, and reliability of events
using data available at any instant estimates
are updated each second - Each user is continuously notified of updated
information . Users computer estimates the
distance of the event, and then calculates an
arrival time, size, and uncertainty - An action is taken when the expected benefit of
the action exceeds its cost - In the presence of uncertainty, false alarms must
be expected and managed
5What we need is a special seismologist
- Someone who has good knowledge of seismology
- Someone who has good judgment
- Someone who works very, very fast
- Someone who doesnt sleep
- We need a Virtual Seismologist
6Virtual Seismologist (VS) method for seismic
early warning
- Bayesian approach to seismic early warning
designed for regions with distributed seismic
hazard/risk - Modeled on back of the envelope methods of
human seismologists for examining waveform data - Shape of envelopes, relative frequency content
- Robust analysis
- Capacity to assimilate different types of
information - Previously observed seismicity
- State of health of seismic network
- Known fault locations
- Gutenberg-Richter recurrence relationship
7Ground motion envelope our definition
Full acceleration time history
Efficient data transmission 3 components each
of Acceleration, Velocity, Displacement, of 9
samples per second
envelope definition max.absolute value over
1-second window
8Data set for learning the envelope
characteristics Most data are from TriNet, but
many larger records are from COSMOS
- 70 events, 2 lt M lt 7.3, R lt 200 km
- Non-linear model estimation (inversion) to
characterize waveform envelopes for these events - 30,000 time histories
9Average Rock and Soil envelopes as functions of
M, R rms horizontal
acceleration
10horizontal acceleration ampl rel. to ave. rock
site
Vertical P-wave acceleration ampl rel. to ave.
rock site
horizontal velocity ampl rel. to ave. rock site
vertical P-wave velocity ampl rel. to ave. rock
site
11Estimating M from ratios of P-wave motions
- P-wave frequency content scales
- with M (Allen and Kanamori, 2003, Nakamura,
1988) - Find the linear combination of log(acc) and
log(disp) that minimizes the variance within
magnitude-based groups while maximizing
separation between groups (eigenvalue problem)
12- Voronoi cells are nearest neighbor regions
- If the first arrival is at SRN, the event must
be within SRNs Voronoi cell - Green circles are seismicity in week prior to
mainshock
13What about Large Earthquakes with Long Ruptures?
- Large events are infrequent, but they have
potentially grave consequences - Large events potentially provide the largest
warnings to heavily shaken regions - Point source characterizations are adequate for
Mlt7, but long ruptures (e.g., 1906, 1857) require
finite fault -
14Strategy to Handle Long Ruptures
- Determine the rupture dimension by using
high-frequencies to recognize which stations are
near source - Determine the approximate slip (and therefore
instantaneous magnitude) by using low-frequencies
and evolving knowledge of rupture dimension - We are using Chi-Chi earthquake data to develop
and test algorithms
15- We are experimenting with different Linear
Discriminant analyses to distinguish near-field
from far-field records
1610 seconds after origin
20 seconds after origin
Near-field Far-field
Near-field Far-field
1730 seconds after origin
40 seconds after origin
Near-field Far-field
Near-field Far-field
18Strategy for acceleration envelopes
- High-frequency energy is proportional to rupture
area (Brune scaling) - Sum envelopes from 10-km patches
19- Sum of 9 point source envelopes
- Vertical acceleration
20- Once rupture dimension is known
- Obtain approximate slip from long-periods
- Real-time GPS would be very helpful
- Evolving moment magnitude useful for estimating
probable rupture length - Magnitude critical for tsunami warning
21Conclusions
- Bayesian statistical framework allows integration
of many types of information to produce most
probable solution and error estimates - Waveform envelopes can be used for rapid and
robust real-time analysis - Strategies to determine rupture dimension and
slip look very promising - User decision making should be based on
cost/benefit analysis - Need to carry out Bayesian approach from source
estimation through user response. In particular,
the Gutenberg-Richter recurrence relationship
should be included in either the source
estimation or user response. - If a user wants ensure that proper actions are
taken during the Big One, false alarms must be
tolerated
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23Distinguishing between P- and S-waves
243 sec after initial P detection at SRN
- Prior information
- Voronoi cells
- Gutenberg-Richter
Single station estimate
M, R estimates using 3 sec observations at SRN
No prior information
8 km M4.4
Note star marks actual M, RSRN
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